Lattice Boltzmann simulations of turbulent channel flow and heat transport by incorporating the Vreman model

Abstract In this article, the Vreman model with a dynamic procedure is applied for subgrid scale modeling of turbulent channel flow and heat transport, under the Lattice Boltzmann framework. Numerical simulations of channel flow at Re τ = 180 with a constant temperature difference at the upper and bottom boundaries are presented and verified via comparisons with existing data of direct numerical simulations and large eddy simulations with the dynamic Smagorinsky model. Additionally, in the same flow and thermal system, the effect of natural convection along the vertical direction is investigated both qualitatively and quantitatively. Results indicate that the bulk velocity is decreased whereas the heat transfer is substantially enhanced. Meanwhile, the vertical thermal convection also alters the profiles of first and second-order statistics, especially in that the temperature fluctuation is flattened in the central region of the channel. Overall, our work offers a useful extension of the current Lattice Boltzmann method in complex situations and will facilitate researches involving turbulent flow and heat transport.

[1]  Y. Qian,et al.  Lattice BGK Models for Navier-Stokes Equation , 1992 .

[2]  T. Zhao,et al.  Lattice Boltzmann modeling of transport phenomena in fuel cells and flow batteries , 2017, Acta Mechanica Sinica.

[3]  Haiqiong Xie,et al.  A lattice Boltzmann model for thermal flows through porous media , 2016 .

[4]  D. Lilly,et al.  A proposed modification of the Germano subgrid‐scale closure method , 1992 .

[5]  Chengwen Zhong,et al.  LES-based filter-matrix lattice Boltzmann model for simulating turbulent natural convection in a square cavity , 2013 .

[6]  Renwei Mei,et al.  Boundary conditions for thermal lattice Boltzmann equation method , 2013, J. Comput. Phys..

[7]  M. J. Pattison,et al.  Computation of turbulent flow and secondary motions in a square duct using a forced generalized lattice Boltzmann equation. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[8]  Ping-Hei Chen,et al.  Numerical implementation of thermal boundary conditions in the lattice Boltzmann method , 2009 .

[9]  L. Luo,et al.  Lattice Boltzmann Model for the Incompressible Navier–Stokes Equation , 1997 .

[10]  P. Moin,et al.  A dynamic subgrid‐scale eddy viscosity model , 1990 .

[11]  P. Moin,et al.  A dynamic subgrid‐scale model for compressible turbulence and scalar transport , 1991 .

[12]  R. Fox Large-Eddy-Simulation Tools for Multiphase Flows , 2012 .

[13]  M. J. Pattison,et al.  Generalized lattice Boltzmann equation with forcing term for computation of wall-bounded turbulent flows. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[14]  A. W. Vreman An eddy-viscosity subgrid-scale model for turbulent shear flow: Algebraic theory and applications , 2004 .

[15]  F. Durst,et al.  Lattice BGK direct numerical simulation of fully developed turbulence in incompressible plane channel flow , 2006 .

[16]  Cyrus K. Aidun,et al.  Lattice-Boltzmann Method for Complex Flows , 2010 .

[17]  P. Moin,et al.  Turbulence statistics in fully developed channel flow at low Reynolds number , 1987, Journal of Fluid Mechanics.

[18]  Jungil Lee,et al.  A dynamic global subgrid-scale model for large eddy simulation of scalar transport in complex turbulent flows , 2012 .

[19]  Sharath S. Girimaji,et al.  LES of turbulent square jet flow using an MRT lattice Boltzmann model , 2006 .

[20]  Chuguang Zheng,et al.  A coupled lattice BGK model for the Boussinesq equations , 2002 .

[21]  Jungil Lee,et al.  A dynamic subgrid-scale eddy viscosity model with a global model coefficient , 2006 .

[22]  Baowei Song,et al.  Improved lattice Boltzmann modeling of binary flow based on the conservative Allen-Cahn equation. , 2016, Physical review. E.

[23]  C. Meneveau,et al.  Scale-Invariance and Turbulence Models for Large-Eddy Simulation , 2000 .

[24]  Sharath S. Girimaji,et al.  DNS and LES of decaying isotropic turbulence with and without frame rotation using lattice Boltzmann method , 2005 .

[25]  P. Moin,et al.  The minimal flow unit in near-wall turbulence , 1991, Journal of Fluid Mechanics.

[26]  B. Shi,et al.  Lattice BGK model for incompressible Navier-Stokes equation , 2000 .

[27]  B. Shi,et al.  Discrete lattice effects on the forcing term in the lattice Boltzmann method. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[28]  Li-Shi Luo,et al.  Lattice Boltzmann simulations of decaying homogeneous isotropic turbulence. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[29]  Z. Tao,et al.  Passive heat transfer in a turbulent channel flow simulation using large eddy simulation based on the lattice Boltzmann method framework , 2011 .

[30]  H. Kawamura,et al.  DNS of turbulent heat transfer in a channel flow with a high spatial resolution , 2009 .

[31]  K. Premnath,et al.  Comparative Study of the Large Eddy Simulations with the Lattice Boltzmann Method Using the Wall-Adapting Local Eddy-Viscosity and Vreman Subgrid Scale Models , 2012 .

[32]  Simulation of a turbulent channel flow with an entropic Lattice Boltzmann method , 2009 .

[33]  Ruey-Jen Yang,et al.  Simulating oscillatory flows in Rayleigh–Bénard convection using the lattice Boltzmann method , 2007 .

[34]  E. Rank,et al.  Extension of a hybrid thermal LBE scheme for Large-Eddy simulations of turbulent convective flows , 2006 .

[35]  M. Germano,et al.  Turbulence: the filtering approach , 1992, Journal of Fluid Mechanics.

[36]  S. Chen,et al.  Comparison of spectral method and lattice Boltzmann simulations of two‐dimensional hydrodynamics , 1993, comp-gas/9303003.

[37]  Haecheon Choi,et al.  Dynamic global model for large eddy simulation of transient flow , 2010 .

[38]  Shiyi Chen,et al.  LATTICE BOLTZMANN METHOD FOR FLUID FLOWS , 2001 .

[39]  M. J. Pattison,et al.  Dynamic subgrid scale modeling of turbulent flows using lattice-Boltzmann method , 2009, 0901.0593.